Semiconducting metal silicide radiation detectors and source

ABSTRACT

Semiconducting metal silicide electromagnetic radiation sources and detectors have a thin film of semiconducting metal silicide grown or deposited on a silicon wafer. The metals are chosen from a group consisting of iron, iridium, manganese, chromium, rhenium, barium, calcium, magnesium and osmium. The detectors are intrinsic semiconductors and can be formed either as discrete devices, or monolithically on a silicon chip to provide an integrated detector or detector array. The semiconducting metal silicide devices are efficient detectors at wavelengths which mate with the transmission capabilities of certain optical fibers enhancing the combination of infra-red detectors and optical fiber transmission preveously known. Iron disilicide is useful as an infra-red radiation source and as an extrinsic detector as well.

FIELD OF THE INVENTION

The present invention relates to a novel electromagnetic radiation detector made from a thin film of iron disilicide and other semiconducting silicide compounds grown or deposited on a silicon wafer or other suitable substrate. The invention relates to the discovery of iron disilicide (FeSi₂), iridium silicide (IrSi₁.75), manganese silicide (MnSi₁.7), chromium disilicide (CrSi₂), rhenium disilicide (ReSi₂), magnesium silicide (Mg₂ Si), barium disilicide (BaSi₂), calcium silicide (Ca₂ Si) and osmium disilicide (OsSi₂) as effective intrinsic electromagnetic radiation detectors and sources. The invention also relates to the combination of these intrinsic electromagnetic radiation detector and devices with electronics on a single chip of an integrated circuit having both electronic data processing and memory and electromagnetic radiation information receiving, processing or transmitting capability. The invented devices can also act as chip interconnects. The present invention is the first to fabricate, and demonstrate the semiconducting nature of, a thin film of rhenium disilicide. All of the above-listed metal silicides except osmium and calcium silicides are effective in the infra-red region. Calcium and osmium silicides are effective in the visible light region of the electromagnetic spectrum.

PROBLEM

It is a problem to fabricate infra-red detectors that are efficient and can be integrated monolithically with other circuitry. Practical devices currently available include intrinsic infra-red semiconductor detectors as discrete devices or linked to electronic circuitry in some form other than on a single silicon chip. Schottky barrier infra-red detectors are also available and workable but are slow for communication purposes and have relatively low quantum efficiency compared to the devices of the present invention. The Schottky barrier devices are of limited wavelength range, they have been integrated successfully in focal plane arrays on a silicon chip.

Silicon intrinsic detectors are effective for visible light and perhaps can be extended in time to wavelengths up to about 0.9 microns. Extrinsic silicon detectors are sensitive to much longer wavelengths, but have absorption coefficients of 1000 to 10,000 times lower than those of intrinsic detectors.

Germanium and germanium-silicon alloys can be grown on a silicon wafer. The absolute long-wavelength limit for germanium based alloys is 1.0 microns and virtually pure germanium has a value of about 1.9 microns. However, germanium and germanium-silicon alloys are relatively weak absorbers of infra-red radiation compared to the transition metal silicide semiconductors described herein. Special structures, such as waveguides, must be developed to use both germanium and germanium-silicon alloys as thin films. The wave guides and other structures are necessary because such devices are weak absorbers of infra-red radiation.

There is also available a family of Mercury-Cadmium-Tellerium devices for infra-red detection. These devices operate without being able to be combined, to date, with an effective microelectronics technology as is possible with silicon based devices.

The devices described above have been effective to some extent. However, there still remains a need for detectors meeting all of the following characteristics: (1) The efficiency of an intrinsic semiconductor detector; (2) Efficient operation in the 1.0 to 14 micron wavelength range; and, (3). Practical fabrication on a silicon chip in a monolithic structure. The need for such devices has been recognized by persons skilled in this art and some attempts have been made recently to fabricate such a device using gallium arsenide (GaAs) and related compounds on a silicon substrate. However, these materials are not currently compatible with silicon processing.

SOLUTION

These problems are solved and a technical advance achieved in the field by the semiconducting metal silicide to devices which are capable of (1) exhibiting decreased electrical resistance or (2) generating a current or voltage when exposed to electromagnetic radiation or (3) emitting electromagnetic radiation when electrical current is passed. These types of devices when exposed to radiation on of suitable wavelength, generate electric current or voltage. When electric current is passed through them, they generate radiation of infra-red or shorter wavelengths depending on the value of the semiconducting energy gap. Iron disilicide now appears to be the one of the above-listed metal silicide radiation sources that exhibits the best performance. Infra-red radiation emitted by these radiation sources ranges in wavelengths from 0.77 microns to 1000 microns.

There are numerous applications for infra-red detectors; one is for terrestrial imaging from space. The limited wavelengths which can be transmitted through the atmosphere are approximately 1.5 to 1.9; 2.0 to 2.6; 3.4 to 4.2; 4.5 to 5.0 and 8 to 13 microns. NASA has shown an interest in the 2.5 to 30 micron wavelength range. Another application for the present invention is in combination with fiber optic systems using silica based fibers (which in long haul, high capacity systems have narrow spectral windows centered on about 1.3 and 1.55 microns). A short haul system has an additional spectral window from about 0.8 to 0.9 microns as well as the windows at about 1.3 and 1.55 microns. In such applications, the output of the infra-red sources can be applied directly to the fiber optics for transmission to an infra-red detector and its associated processor. Since the intrinsic electromagnetic radiation detector and source devices are silicon-compatible, they can be combined on the same chip as other silicon based elements such as data storage and data processing elements. In such a combination, the signal processing and related computing can be performed on the very same chip that holds the source, detector, imaging or detector array. Monolithic systems afford many advantages compared to hybrid systems.

The detectors can be arranged singly or in an array. A two dimensional array can be constructed. Each element in the array has an output which can converted into a digital electrical signal.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a perspective view of one embodiment of the present invention showing a metal silicide semiconductor infra-red radiation detector.

FIG. 2 shows a view of a circuit using the detector shown in FIG. 1.

FIG. 3 shows an array of devices shown in FIG. 1 forming another embodiment of the present invention.

FIG. 4 shows an array of devices, as shown in FIG. 3, formed on a common silicon substrate with a very large scale integrated circuit forming another embodiment of the present invention.

FIG. 5 shows an array of semiconducting metal silicide infra-red detectors arranged in an array to mate with a bundle of optical fibers forming still another embodiment of the present invention.

FIG. 6 is a perspective view of another embodiment of the present invention showing the metal silicide layer deposited directly on the silicon substrate.

FIG. 7 shows an array of metal silicide semiconducting infra-red detectors arranged to mate with an array of optical fibers forming still another embodiment of the present invention.

FIG. 8 shows a perspective view of a semiconducting metal silicide homojunction radiation source and detector forming another embodiment of the present invention.

FIG. 9 is a perspective view of a semiconducting metal heterojunction silicide infra-red radiation source and detector forming another embodiment of the present invention.

FIG. 10 is a chart showing the optical absorption coefficient of several of the metal silicide semiconductors invented herein as a function of wavelength in microns. The chart also shows some practical wavelength ranges of optical fibers, the atmospheric windows of terrestrial infra-red radiation and NASA's indicated range of interest.

FIG. 11 shows chip intraconnects in which one metal silicide semiconducting device is connected to another metal silicide semiconducting device on the same chip.

FIG. 12 shows chip interconnects in which one metal silicide semiconducting device is connected to another metal silicide semiconducting device on a different chip with or without the use of a fiber optic line.

DESCRIPTION OF THE INVENTION

FIG. 1 shows a perspective view of one embodiment of the present invention being formed of a semiconducting metal silicide shown by the numeral 10. The substrate 12 is a silicon wafer thermally oxidized to grow 1000 angstroms more or less of insulating oxide 14. The oxide layer 14 is then coated with several thousand angstroms of polycrystalline silicon film 16. This polycrystalline silicon film is added commonly by low pressure vapor deposition. A thin film of metal is then added to the polycrystalline silicon film 16 and then reacted by heating the sample in an inert environment to react the metal film with the layer below to form a semiconducting metal silicide 18. Electrical contact with the semiconducting metal silicide is achieved by depositing an aluminum or other conductive film 20, 22 and 24 on the semiconducting metal silicide which is then photolithographically patterned. Other insulating substrates can be used and coated with a silicon film. The metal deposition technique can be evaporation or chemical vapor deposition. Furthermore, the silicide film may be formed by (simultaneous) codeposition of metal and silicon.

FIG. 6 shows a another embodiment of the present invention having a substrate 120 on top of which is formed a thin film metal silicide 180. Conductive pads 121, 122 and 140 are formed on the surface of the thin film metal silicide 180.

The metal can be chosen from the group consisting of: iron, iridium, manganese, chromium, rhenium, magnesium, calcium, barium or osmium. The silicides formed are: iron disilicide (FeSi₂), iridium silicide (IrSi₁.75), manganese silicide (MnSi₁.7), chromium disilicide (CrSi₂), rhenium disilicide (ReSi₂), magnesium silicide (Mg₂ Si), barium disilicide (BaSi₂), calcium silicide (Ca₂ Si) or osmium disilicide (OsSi₂) respectively.

The process for forming each metal silicide should vary as to annealing temperature and time. The chart 1 shown below shows the time, temperature and a range of thickness for the metal silicides. Each metal silicide thus made has been tested and shown to be a true semiconductor which demonstrates useful radiation detection properties based either on analysis of the data showing the optical absorbtion edge for each material together with measurements of electrical resistivity as a function of temperature. Iron disilicide is a photoconductive infra-red detector.

                  CHART 1                                                          ______________________________________                                         Element  Temp./Time (minutes)                                                                            Thickness (Angstroms)                                ______________________________________                                         Chromium 900 C./120-1100 C./120                                                                          1000-13,000                                          Manganese                                                                               800 C./120-1000 C./60                                                                           1900-15,000                                          Iridium  750 C./120-850 C./120                                                                           1355-5,418                                           Rhenium  900 C./120       307-768                                              Iron     900 C./120       700-3,200                                            ______________________________________                                    

The data showing the optical absorption edges for various materials are shown in Appendix "A" which consists of figures showing data for iron disilicide, manganese silicide, chromium disilicide, iridium silicide and rhenium disilicide.

The silicide layer can be made by depositing a thin film of the desired metal onto a silicon wafer which has been polished and cleaned for integrated circuit fabrication. It is important to have a clean metal-silicon interface before annealing. After heating to the proper temperature and for the proper time, the metal film will react with the silicon substrate to form a metal silicide semiconductor. The semiconducting metal silicide film may also be grown on a polycrystalline silicon surface.

For example, rhenium disilicide (ReSi₂) was prepared by ion beam sputtering of rhenium film onto 1-0-0 polished silicon wafers. The silicide layer was grown by reaction of the metal film with the silicon substrate at 900 degrees C. in an inert environment of flowing argon gas. The substrate is ion-milled in vacuum immediately prior to metal deposition. Appendix "B" attached hereto and forming a part of this application gives a detailed description of the fabrication of iron disilicide. A similar process is used for the formation of the other semiconducting metal silicides with annealing times and temperatures varying in a similar fashion as set forth in Chart 1. Naturally, variations of these parameters are certainly possible even for those materials listed in Chart 1.

FIG. 2 shows a circuit used with the device shown in FIG. 1. The conductive pads 20, 22 formed on the semiconducting metal silicide layer shown in FIG. 1 are by wires 21, 23 connected to a current source 50. Conductive pads 24 of FIGS. 1 are connected by wires 25, 27 to a voltmeter 60. A source of infra-red radiation 70 illuminates semiconducting metal silicide device 10. The resistance of the metal silicide device 10 drops as it is exposed to radiation so that the voltage detected by voltmeter 60 drops as a function of the intensity of infra-red radiation from infra-red radiation source 70. An analog-to-digital converter 62 is shown receiving information from voltmeter 60 for digitizing the output of the metal silicide infra-red detector.

FIG. 3 shows an array of devices of the type shown in FIG. 1. The array shown generally by the number 300 is formed of twenty-five metal silicide semiconductors 302. Each semiconducting metal silicide device 302 has leads 304 into which a constant current can be fed from a current source (not shown). Each semiconducting metal silicide device 302 also has leads 306 from which the voltage drop across the semiconducting metal silicide device can be measured or detected. The array 300 is grown on a substrate 308 which can be formed of a wide variety of materials including silicon. If silicone is the chosen substrate, the entire array can be formed monolithically. In that case the leads 304, 306 would be formed on the substrate photolithography by techniques well known in the semiconductor fabricating industry.

FIG. 4 shows an integrated circuitry array 101 formed of microprocessor circuitry 100 (or other VLSI device) and a metal silicide semiconductor infra-red detector array 110 shown for the purposes of illustration only as a separate element. One use of such a device is incoming missile detection and ranging. Currently, such combinations of infra-red detection and computer analysis of the incoming signals are performed by interconnecting discrete devices. The discrete devices each perform satisfactorily but are not as fast, compact, low cost to make, or reliable as a single integrated device. The potential speed difference is substantial, perhaps 100 times that of present devices. The quality of the electrical interconnects is an important factor in the speed of the device. Similarly, the integrated system is more rugged, faster and more reliable than a hybrid system formed of discrete devices. The net result is that the integrated system could be hand held or easily portable. The increased speed of date processing, the ruggedness and reliability can be critical in military and space use.

FIG. 4 shows the array as a two dimensional array of semiconducting metal silicide source devices 12 whose output is represented by the bundle of leads 112 which contain data fed to microprocessor circuitry 100. Microprocessor circuitry 100 fabricated on substrate 106 receives power through leads 102 and transmits information via leads 104. Additional data and control information may be placed into the microprocessor 100 by leads 108. The entire integrated circuit 105 is fabricated on a substrate 106 typically of silicon.

FIG. 5 shows a bundle of optical fibers 200 which are aligned with and receive signals from a mating array 210 of semiconducting metal silicide sources 12. The direction of transmission can be reversed so that the fiber optic bundle 200 transmit radiation to an array of semiconducting metal silicide detectors 12. While devices can in some cases operate as sources, in practice devices will be optimized for each application as either sources or detectors.

FIG. 7 shows a linear array 309 of semiconducting metal silicide detectors 313, 311 and 303 having leads 305 and 307 for receiving current and for connecting to instruments for measuring changed resistance, photocurrent or photovoltage. The array 309 is mated with an array of optical fibers 325 having, for example, three fibers 203, 211 and 213 which align with elements 303, 311 and 313 as shown in the figure.

For instance, while it is known that all of the metal silicides described herein can function as radiation sources, because of the direct band gap of FeSi₂, it is apparent that FeSi₂ will function as a radiation source.

The functioning of the semiconducting metal silicide devices as interconnecting or intraconnecting devices will facilitate high speed communications and data processing. It is well known that a major limitation to achieve significant speed increases in VLSI and has been the inherent limitations in metallic connections.

FIG. 8 shows in detail a substrate 401 which can be formed of either p- or n-type silicon has two layers of either n or p type doped silicide 402 and 404 formed thereon. The upper and lower metal silicide layers must be oppositely doped material and the base should be opposite in doping to the layer adjacent to it as shown in FIG. 8. Part of the upper layer 406 is removed to expose the surface 410 of the lower layer of semiconducting metal silicide 402. Conductive contacts 408 are formed on both surfaces 406 and 410 for permitting electrical connection to the device. Current is injected at lead 413 and removed at lead 415 or vice versa for operation as a source of electromagnetic radiation. When exposed to electromagnetic radiation, the device may generate a photocurrent "i" or alternatively a photovoltage between leads 408 and 406.

FIG. 9 shows another embodiment in the form of a heterojunction device 500 having a silicon substrate 501 and a metal silicide thin film 502. Conductive contacts 514 and 516 are formed on the bottom of the substrate and the top of the silicide thin film, respectively. Current is injected at 512 and removed at 510 or vice versa for operation as a source of electromagnetic radiation. When exposed to electromagnetic radiation, the device may generate a photocurrent "i" or alternatively a photovoltage between leads 510 and 517.

FIG. 10 is a graph showing the optical absorption coefficient for the inventive semiconducting metal silicides as a function of wavelength. Superimposed on the graph are practical wavelength windows of terrestrial infra-red radiation, the windows of transmission of optical fibers and NASA's range of interest for extra-terrestrial instrumentation.

FIGS. 11 and 12 show two further embodiments of the present invention. FIG. 11 shows an integrated circuit element 551 formed on a substrate 552, which typically is silicon. Two other circuit elements 554, 556 illustrate circuit elements fabricated on the substrate 552, such circuit elements 554, 556 may, for instance, transfer data from one to the other such as two memory elements. Element 554 conveys its information to radiation source 557 which emits a pulse of energy at output 560 which is carried by waveguide 564 formed monolithically on surface 552 to detector 562 which converts the radiation signal to an electric current through leads 558 which carries it to element 556.

FIG. 12 shows an embodiment similar to that of FIG. 11, except that in FIG. 12 the circuit elements 576, 582 are mounted or formed on separate chips 574, 580. FIG. 11 shows a chip intraconnect; FIG. 12 shows chip interconnects. Interconnected chips 574, 580 include circuit elements 576, 582 and metal silicide devices as both sources and detectors 578, 584 and elements, such as memory elements 576, 582. Communication between chips 574, 580 is achieved, for instance, through photosource 578 and photodetector 584 as described above for FIG. 11. The photosource 578 and photodetector 584 may communicate through an air-gap or through a fiber optic channel 586 which is mounted to interconnect the chips 574, 580. Naturally such communication can be bi-directional.

The thickness of the various film layers varies for each material. Rhenium disilicide layers were formed of thickness of about 307, 461 and 768 angstroms; manganese silicide (MgSi₁.7) samples were formed with thicknesses ranging from about 1,900 to about 15,100 angstroms. Chromium disilicide samples were formed with layers of about 1,600; 4,300, 5,647 and 13,455 angstroms. These and other thicknesses are shown in the chart produced earlier. In fact, thickness ranging from about 100 angstrom to about 50,000 angstroms should be obtainable.

While a specific embodiment of this invention has been disclosed herein, it is expected that those skilled in the art can design other embodiments that differ from this particular embodiment but fall within the scope of the amended claims. 

What I claim is:
 1. An integrated circuit comprising:a silicon substrate means; monolithic circuit means deposited on said silicon substrate means and having a portion formed of a semiconductive metal silicide means and a portion formed of any other silicon compatible semiconducting means.
 2. The integrated circuit of claim 1 wherein:said metal is selected from the group consisting of: iron, iridium, manganese, chromium, rhenium, calcium, barium, magnesium or osmium.
 3. The integrated circuit of claim 1 wherein:said monolithic circuit means includes at least one processor means electrically connected to said semiconductive metal silicide means.
 4. The integrated circuit of claim 1 including further:a conductive means formed in a pattern on said semiconductive metal silicide means to form an array of detector members and to interconnect said array of detector members to said monolithic circuit means.
 5. The integrated circuit of claim 4 including further:a plurality of fiber optic radiation carriers mated to said array of detector members to provide data to said array of detector members.
 6. The integrated circuit of claim 1 including further:a conductive means formed in a pattern on said semiconductive metal silicide means to interconnect a plurality of source members to form an array of source members and to interconnect said array of source members to said monolithic circuit means; a plurality of fiber optic radiation carriers mated to said array of source members to carry data away from said array of source members.
 7. A radiation detector comprising:a p- or n-type substrate means; a first thin film of semiconductive metal silicide deposited on said substrate means and doped with a type of dopant opposite to that of said substrate means; a second thin film of semiconductive metal silicide deposited on said first thin film and doped with a type of dopant the same as that of said substrate means; first and second electrically conducting means formed on said first and second thin films respectively.
 8. The radiation detector of claim 7 wherein:the metal is chosen from the group consisting of: iron, iridium, manganese, chromium, rhenium, calcium, barium, magnesium or osmium.
 9. The radiation detector of claim 7 wherein:the metal silicide is chosen from the group consisting of: iron disilicide (FeSi₂), iridium silicide (IrSi₁.75), manganese silicide (MnSi₁.7), chromium disilicide (CrSi₂), rhenium disilicide (ReSi₂), magnesium silicide (Mg₂ Si), barium disilicide (BaSi₂), calcium silicide (Ca₂ Si) and osmium disilicide (OsSi₂).
 10. An infra-red radiation detector comprising in combination:a thin film of semiconductive metal silicide; a silicon substrate means; first and second conductive means formed on said thin film of semiconductive metal silicide and on said silicon substrate means respectively.
 11. The device of claim 10 wherein said metal silicide is chosen from the group consisting of: iron disilicide (FeSi₂), iridium silicide (IrSi₁.75), manganese silicide (MnSi₁.7), chromium disilicide (CrSi₂), rhenium disilicide (ReSi₂), magnesium silicide (Mg₂ Si), barium disilicide (BaSi₂), calcium silicide (Ca₂ Si) and osmium disilicide (OsSi₂).
 12. An integrated circuit comprising in combination:a substrate means; first and second circuit means formed on said substrate means in which the second circuit means receives data from the first circuit means; first and second semiconductive metal silicide means formed on said substrate means; the first and second semiconductive metal silicide means interconnected electrically to said first and second circuit means respectively; the first semiconductive metal silicide means having radiation emitting properties; the second semiconductive metal silicide means having radiation detecting properties; waveguide means formed on said substrate means for interconnecting said first and second semiconductive metal silicide means.
 13. An integrated circuit comprising in combination:first and second substrate means; first and second circuit means formed on said first and second substrate means respectively in which said second circuit means receives data from said first circuit means; first and second semiconductive metal silicide means formed on said first and second substrate means respectively: the first and second semiconductive metal silicide means interconnected electrically to said first and second circuit means respectively; the first semiconductive metal silicide means having radiation emitting properties; the second semiconductive metal silicide means having radiation detecting properties.
 14. An integrated circuit comprising in combination:first and second substrate means; first and second circuit means formed on said first and second substrate means respectively in which the second circuit means receives data from said first circuit means; first and second semiconductive metal silicide means formed on first and second substrate means respectively: the first and second semiconductive metal silicide means interconnected electrically to the first and second circuit means respectively; the first semiconductive metal silicide means having radiation emitting properties; the second semiconductive metal silicide means having radiation detecting properties; waveguide means for interconnecting said first and second semiconductive metal silicide means.
 15. A device comprising the composite structure of:substrate means; a layer of semiconductive metal silicide deposited or grown on said substrate means.
 16. The device of claim 15 wherein said metal is selected from the group consisting of: iron, iridium, manganese, chromium, rhenium, calcium, barium, magnesium, or osmium.
 17. The device of claim 15 wherein said substrate means is selected from the group consisting of: silicon, glass, quartz, sapphire or ceramic.
 18. A photoconductive detector device for detecting electromagnetic radiation comprising the device of claim 16 in combination with:first and second electrically conductive means formed on said layer of semiconductive metal silicide for making ohmic contact with said layer of semiconductive metal silicide; means for directing electromagnetic radiation on said layer of semiconductive metal silicide.
 19. The device of claim 18 wherein said layer of semiconductive metal silicide is responsive to infra-red light applied to it by said directing means for exhibiting a reduction in the resistance of said layer of semiconductive metal silicide between said first and said second electrically conductive means.
 20. The device of claim 15 wherein said metal is selected from the group consisting of: iron, manganese.
 21. A device for generating infra-red electromagnetic radiation comprising the device of claim 20 in combination with:first electrically conductive means deposited on a surface of said substrate for making ohmic contact with said substrate; second electrically conductive means deposited on a surface of said layer of semiconductive metal silicide for making ohmic contact with said layer of semiconductive metal silicide; means for applying a source of electrical potential across said first and said second electrically conductive means.
 22. A device comprising the composite structure:a substrate means; a thin film of semiconductive metal silicide deposited on a surface of said substrate means.
 23. The device of claim 22 wherein the metal is selected from the group consisting of: iron, iridium, manganese, chromium, rhenium, calcium, barium, magnesium or osmium.
 24. A device for detecting electromagnetic radiation comprising the device of claim 23 in combination with:first and second electrically conductive means deposited on said thin film of semiconductive metal silicide for making ohmic contact with said thin film of semiconductive metal silicide; means for directing light radiation on said thin film of semiconductive metal silicide.
 25. The device of claim 22 wherein said thin film of semiconducting metal silicide comprises a thin film of rhenium disilicide.
 26. The device of claim 25 wherein the thickness of said thin film of rhenium disilicide was approximately 307 to 768 Angstroms.
 27. The device of claim 22 wherein the metal is selected from the group consisting of: iron or manganese.
 28. A device for generating infra-red radiation comprising the device of claim 27 in combination with:first electrically conductive contact deposited on said substrate means for making ohmic contact with said substrate means; second electrically conductive contacts deposited on said thin film of semiconductive metal silicide for making ohmic contact with said thin film of semiconductive metal silicide; means for applying an electrical potential to said first and said second electrically conductive contacts.
 29. The device of claim 22 further comprising:integrated circuit means formed on said surface of said substrate means; two or more electrically conductive means ohmically connected to and electrically interconnecting said integrated circuit means and said thin film of semiconductive metal silicide.
 30. The device of claim 15 wherein said semiconductive metal silicide is chosen from the group comprising: iron disilicide (FeSi₂), iridium silicide (IrSi₁.75), manganese silicide (MnSi₁.7), chromium disilicide (CrSi₂), rhenium disilicide (ReSi₂), magnesium silicide (Mg₂ Si), barium disilicide (BaSi₂), calcium silicide (Ca₂ Si) and osmium disilicide (OsSi₂).
 31. A photoconductive detector device for detecting electromagnetic radiation comprising the device of claim 16 in combination with:first electrically conductive means formed on said layer of semiconductive metal silicide for making ohmic contact with said layer of semiconductive metal silicide; said electrically conductive means formed on said layer of semiconductive metal silicide for making a rectifying contact with said layer of semiconductive metal silicide; means for directing electromagnetic radiation on said layer of semiconductive metal silicide.
 32. A radiation source comprising:a p- or n-type substrate means; a first layer of semiconductive metal silicide deposited or grown on said substrate means and doped with a type of dopant opposite to that of said substrate means; a second layer of semiconductive metal silicide deposited or grown on and partly overlaying said first layer and doped with a dopant the same as that of said substrate means; first and second electrically conducting means formed on said first and second layers respectively. 